243-284 | The theory of the Taylor dispersion technique for liquid diffusivity measurements | A. Alizadeh, C. A. Nieto de Castro and W. A. Wakeham |
285-298 | The three-parameter corresponding states principle | G. A. Mansoori, V. K. Patel and M. Edalat |
299-315 | Anharmonic effects in the specific heat of aluminum | R. C. Shukla and C. A. Plint |
317-326 | Specific heat capacity and electrical resistivity of a carbon-carbon composite in the range 1500–3000 K by a pulse heating method | A. Cezairliyan and A. P. Miiller |
331-344 | Transport properties of nonelectrolyte liquid mixtures—I. Viscosity coefficients for n-alkane mixtures at saturation pressure from 283 to 378 K | J. H. Dymond and K. J. Young |
345-373 | Transport properties of nonelectrolyte liquid mixtures—II. Viscosity coefficients for the n-hexane + n-hexadecane system at temperatures from 25 to 100‡C at pressures up to the freezing pressure or 500 MPa | J. H. Dymond, K. J. Young and J. D. Isdale |
375-381 | Thermal conductivity of nitrogen at high pressures | R. Tufeu and B. Neindre |
383-396 | Pressure-density-temperature measurements of ethylene | W. Thomas and M. Zander |
397-416 | Correlation of the transport properties of simple fluids at low temperatures and high pressures based on the generalized Eucken relation and the molecular dynamics of hard sphere fluid | T. H. Chung, L. L. Lee and K. E. Starling |
417-427 | Electrical resistivity of molybdenum in the temperature range 1500 to 2650 K | A. Cezairliyan |
1-19 | Behavior of a nonconformal mixture via computer simulation | H. J. M. Hanley and D. J. Evans |
21-38 | Organic liquid thermal conductivity: A prediction method in the reduced temperature range 0.3 to 0.8 | C. Baroncini, P. Filippo, G. Latini and M. Pacetti |
39-54 | Thermal diffusivity of liquids determined by flash heating of a three-layered cell | M. M. Farooq, W. H. Giedt and N. Araki |
55-62 | Theory of lattice thermal conductivity: Role of low-frequency phonons | P. G. Klemens |
63-70 | The melting point of palladium by a pulse heating method | A. P. Miiller and A. Cezairliyan |
71-87 | The effect of impurities on the melting temperature and the heat of fusion of latent heat storage materials | J. Sohns, B. Seifert and E. Hahne |
89-101 | Influence of the size factor on the thermal shock resistance of ceramic samples | J. C. Glandus and P. Boch |
301-314 | The viscosity of aqueous KCl solutions in the temperature range 25–200°C and the pressure range 0.1–30 MPa | J. Kestin, I. R. Shankland and R. Paul |
315-322 | The viscosity of Na2CO3 and K2CO3 aqueous solutions in the range 20–60°C | F. A. Gonçalves and J. Kestin |
323-330 | Thermal conductivity of pure monoisotopic silicon | P. G. Klemens |
331-340 | Thermal conductivity and heat capacity of solid silver bromide (AgBr) under pressure | R. G. Ross and P. Andersson |
341-353 | The influence of neutron irradiation on the thermal conductivity of aluminum in the range 5–50 K | H. Misiorek, T. Zakrzewski and J. Rafalowicz |
357-370 | Variances in the measurement of thermal diffusivity on coarse-weave carbon-carbon composites in terms of fiber-fraction involvement | M. S. Deshpande, R. H. Bogaard and R. E. Taylor |
371-380 | Contributions to the heat capacity of alpha (HCP) titanium from 200–1000 K | C. R. Brooks |
381-394 | Near infrared absorption coefficient of molten glass by emission spectroscopy | J. I. Berg |
101-116 | Thermal conductivity of fourteen liquids in the temperature range 298–373 K | H. Kashiwagi, M. Oishi, Y. Tanaka, H. Kubota and T. Makita |
117-135 | Thermal conductivity of oxygen in the critical region | L. A. Weber |
137-155 | Experimental determination of the volume change of pure salts and salt mixtures at their melting point | J. P. Petitet, M. Fraiha, R. Tufeu and B. Neindre |
157-164 | Thermodynamic characteristics of vaporization of alkali metals | M. M. Stevanović |
165-200 | Enthalpy and heat capacity of the actinide oxides | J. K. Fink |
201-215 | Thermal conductivity and density of toluene in the temperature range 273–373 K at pressures up to 250 MPa | H. Kashiwagi, T. Hashimoto, Y. Tanaka, H. Kubota and T. Makita |
217-224 | Thermal conductivity of n-tridecane at pressures up to 500 MPa in the temperature range 35–75°C | M. Mustafa, M. Sage and W. A. Wakeham |
225-235 | A transient hot-wire instrument for thermal conductivity measurements in electrically conducting liquids at elevated temperatures | A. Alloush, W. B. Gosney and W. A. Wakeham |
237-249 | Measurements of the viscosity of compressed gaseous and liquid nitrogen + methane mixtures | D. E. Diller |
251-257 | Heat capacity of fcc calcium | G. Grimvall and J. Rosén |
259-288 | Transient interferometric technique for measuring thermal expansion at high temperatures: Thermal expansion of tantalum in the range 1500–3200 K | A. P. Miiller and A. Cezairliyan |
289-305 | Viscosity of twelve hydrocarbon liquids in the temperature range 298–348 K at pressures up to 110 MPa | H. Kashiwagi and T. Makita |
307-323 | Mutual diffusion coefficients for binary mixtures of normal alkanes | A. A. Alizadeh and W. A. Wakeham |
325-334 | Vapor-liquid equilibrium measurements on benzene + n-decane systems at 298.15 and 323.15 K | R. G. Rubio, J. A. R. Renuncio and M. Diaz Peña |
335-364 | Experimental and theoretical studies of the influence of surface conditions on radiative properties of opaque materials | P. Demont, M. Huetz-Aubert and H. Tran N'Guyen |
365-369 | Shear viscosity of the binary liquid mixture 3-methylpentane + nitroethane near the consolute point | C. M. Sorensen |
1-10 | Thermal conductivity of carbon disulphide at pressures up to 500 MPa | U. V. Mardolcar and W. A. Wakeham |
11-33 | Thermal conductivity measurement of n-butane over wide temperature and pressure ranges | C. A. Nieto de Castro, R. Tufeu and B. Neindre |
35-50 | Determination of the thermodynamic properties of water from measurements of the speed of sound in the temperature range 251.15–293.15 K and the pressure range 0.1–350 MPa | J. P. Petitet, R. Tufeu and B. Neindre |
51-95 | A switch function applied to the thermodynamic properties of steam near and not near the critical point | H. W. Woolley |
97-114 | Pressure tensor and viscosity coefficients of a soft sphere liquid under shear | S. Hess and H. J. M. Hanley |
115-125 | Measurement of thermal conductivity, heat capacity, and thermal diffusivity of sulfur and selenium in the liquid state | A. A. El-Sharkawy and M. T. Dessouky |
127-138 | Evaluation of P-V-T-composition characteristics of carbon saturated vapor | M. M. Stevanović |
139-147 | Vibrational entropy of polyatomic solids: Metal carbides, metal borides, and alkali halides | G. Grimvall and J. Rosén |
149-157 | Correction of specific heat in isobaric expansion data | G. R. Gathers |
159-171 | Measurement of the heat capacity of molybdenum (Standard Reference Material) in the range 1500–2800 K | A. Cezairliyan |
173-181 | Heat capacity and electrical resistivity of SRM molybdenum (1300–2500 K) | F. Righini and A. Rosso |
183-188 | Thermal conductivity of LaCoO3 | C. G. S. Pillai and A. M. George |
189-192 | In Memoriam: Dr. Charles W. Beckett (1907–1983) | David Garvin, Stanley Abramowitz and Ared Cezairliyan |
193-208 | Thermal conductivity of five hydrocarbons along the saturation line | J. C. G. Calado, J. M. N. A. Fareleira, C. A. Nieto de Castro and W. A. Wakeham |
209-226 | Thermophysical properties of liquid copper and aluminum | G. R. Gathers |
227-233 | Solid and liquid lithium enthalpy: Experimental investigation near the melting point | I. I. Novikov, V. V. Roschupkin and L. C. Fordeyeva |
235-252 | High speed scanning calorimetry for amorphous alloys | B. Hopstadius and G. BÄckström |
253-259 | Melting curve of o-terphenyl | V. J. Fratello and V. E. Bean |
261-269 | Thermophysical properties of polycrystalline PbS, PbSe, and PbTe in the temperature range 300–700 K | A. A. El-Sharkawy, A. M. Abou El-Azm, M. I. Kenawy, A. S. Hillal and H. M. Abu-Basha |
271-278 | Electrical resistivity and thermal expansion of liquid titanium and zirconium | G. R. Gathers |
279-282 | Announcements |
3-4 | Introduction | A. Cezairliyan and J. V. Sengers |
5-12 | Japanese research on thermophysical properties of fluids | A. Nagashima |
13-21 | Japanese research on thermophysical properties of solids | K. Kobayasi |
23-40 | Thermophysical properties of liquids at high pressures | T. Makita |
41-52 | Measurement of thermophysical properties of metals and ceramics by the laser-flash method | Y. Takahashi |
53-71 | Measurements of thermophysical properties by a stepwise heating method | N. Araki |
73-90 | Present status of research on radiative properties of materials | T. Kunitomo |
91-110 | Reference materials and evaluation of thermophysical properties data | K. Iizuka, A. Ono and K. Yoshida |
111-112 | Announcements |
241-263 | Viscosity of aqueous NaCl solutions in the temperature range 25–200 °C and in the pressure range 0.1–30 MPa | J. Kestin and I. R. Shankland |
265-279 | Thermal conductivity of methane | R. C. Prasad, N. Mani and J. E. S. Venart |
281-290 | Accurate measurements of the PVT properties of methane from —20 to 150 °C and to 690 MPa | E. C. Morris |
291-300 | Thermal pressure coefficients of ethanenitrile, propanenitrile, and butanenitrile in the region 295–395 K | I. A. McLure and J. L. Arriaga-Colina |
301-313 | Thermal and electrical conductivities of an improved 9 Cr-1 Mo steel from 360 to 1000 K | R. K. Williams, R. S. Graves and D. L. McElroy |
315-320 | Melting temperature of nickel by a pulse heating technique | A. Cezairliyan and A. P. Miiller |
321-322 | 9th symposium on thermophysical properties Boulder, Colorado, U.S.A. June 24–27, 1985 |
321 | Important announcement | |
323-350 | Thermal conductivity of hydrogen for temperatures between 78 and 310 K with pressures to 70 MPa | H. M. Roder |
351-365 | Thermal conductivity of benzene and cyclohexane in the temperature range 36–90°C at pressures up to 0.33 GPa | S. F. Y. Li, G. C. Maitland and W. A. Wakeham |
367-385 | Thermal conductivity of ethane from 290 to 600 K at pressures up to 700 bar, including the critical region | R. C. Prasad and J. E. S. Venart |
387-401 | Thermal conductivity of organic liquid binary mixtures: Measurements and prediction method | C. Baroncini, G. Latini and P. Pierpaoli |
403-429 | Contributions to the heat capacity of solid molybdenum in the range 300–2890 K | A. Choudhury and C. R. Brooks |
431-432 | Announcements |
1 | Editor's note | Ared Cezairliyan |
3-20 | Thermal conductivity of carbon tetrafluoride with argon and helium | N. Imaishi, J. Kestin and R. Paul |
21-41 | Transport properties of nonelectrolyte liquid mixtures—VI. Viscosimetric study of binary mixtures of hexafluorobenzene with aromatic hydrocarbons | J. H. Dymond and J. Robertson |
43-62 | Measurements of the viscosities of saturated and compressed liquid normal butane and isobutane | D. E. Diller and L. J. Poolen |
63-82 | Equation of state for liquid helium from 1.4 to 4 K and asymptotic limits at the lamda line | V. Arp and K. Agatsuma |
83-99 | Changes in seebeck coefficient of Pt and Pt 10% Rh after use to 1700°C in High-purity polycrystalline alumina | R. E. Bentley |
101-105 | Specific heat capacity of solids under pressure from measurements of (∂T/∂P)s | G. Bäckström and R. G. Ross |
107 | Important announcement |
107-118 | Thermal conductivity of sulfur hexafluoride | J. Kestin and N. Imaishi |
119-142 | Thermal conductivity of methane for temperatures between 110 and 310 K with pressures to 70 MPa | H. M. Roder |
143-163 | Thermal accommodation coefficient of gases on controlled solid surfaces: Argon-tungsten system | S. C. Saxena and R. Afshar |
165-175 | Automated differential scanning calorimetry at low temperatures | Å. Fransson and G. Bäckström |
177-190 | Thermal conductivity and heat capacity of solid nabr under pressure | I. Sigalas, B. Håkanson and P. Andersson |
191-202 | Thermophysical measurements on tungsten-3 (wt %) rhenium alloy in the range 1500–3600 K by a pulse heating technique | A. Cezairliyan and A. P. Miiller |
315-330 | Experimental determination of the thermal conductivity of molten pure salts and salt mixtures | R. Tufeu, J. P. Petitet, L. Denielou and B. Neindre |
331-351 | p, V, T and derived thermodynamic data for toluene, trichloromethane, dichloromethane, acetonitrile, aniline, and n-dodecane | A. J. Easteal and L. A. Woolf |
353-365 | Thermal conductivity of solid NaF under high pressure | B. Håkansson and R. G. Ross |
367-393 | Critical evaluation of the thermodynamic properties of molybdenum | A. Fernández Guillermet |
395-409 | Evaluation of the thermodynamic properties of tungsten | P. Gustafson |
411-419 | Thermodynamic properties of chromium | J. -O. Andersson |
421-426 | Point-defect formation and temperature coefficient of electrical resistivity of platinum and platinum-(10 wt%) rhodium alloy in the range 1100–1900 K | S. Yu. Glazkov |
1007-1021 | Dilute-gas properties of the monatomic gases and their mixtures from the MSK potential | W. Ameling and K. Lucas |
1023-1031 | A new correlation for the viscosity of gaseous fluorocarbon refrigerants | K. Nagaoka, Y. Tanaka, H. Kubota and T. Makita |
1033-1051 | Hydrogen component fugacities in binary mixtures with methane and propane | T. J. Bruno, G. L. Hume and J. F. Ely |
1053-1063 | Hydrogen component fugacities in binary mixtures with carbon dioxide | T. J. Bruno and G. L. Hume |
1065-1075 | Velocity of sound in supercritical water up to 700°C and 300 MPa | J. P. Petitet, L. Denielou, R. Tufeu and B. Neindre |
1077-1089 | PVT properties of methanol at temperatures to 300°C | G. C. Straty, A. M. F. Palavra and T. J. Bruno |
1091-1100 | Thermal conductivity of La2CuO4, La2NiO4, and Nd2CuO4 in the semiconducting and metallic phases | C. G. S. Pillai and A. M. George |
1101-1113 | Spectral radiative properties of a living human body | N. Terada, K. Ohnishi, M. Kobayashi and T. Kunitomo |
1115-1133 | Improved tables for the calculation of nonspherical contributions to second virial coefficients | A. Boushehri, E. A. Mason and J. Kestin |
1135-1145 | Correlation and extrapolation of dilute-gas properties of simple linear molecules with the SSR-MPA potential model | W. Ameling and K. Lucas |
1147-1161 | Thermal conductivity and heat capacity of liquid toluene at temperatures between 255 and 400 K and at pressures up to 1000 MPa | V. M. Shulga, F. G. Eldarov, Yu. A. Atanov and A. A. Kuyumchev |
1163-1182 | Specific heats (Cv) of saturated and compressed liquid and vapor carbon dioxide | J. W. Magee and J. F. Ely |
1183-1190 | Corrections to the electronic heat capacity of metals due to finite lifetimes of the conduction electrons | M. Thiessen |
1191-1208 | Stratified media theory interpretation of measurements of the spectral polarized directional emissivity of some oxidized metals | J. M. Ane and M. Huetz-Aubert |
407-414 | Thermal conductivity of oct-1-ene in the temperature range 307 to 360 K at pressures up to 0.5 GPa | S. F. Y. Li, W. A. Wakeham and M. Zalaf |
415-424 | Solid-liquid phase equilibria of benzene + cyclohexane system under high pressures | K. Nagaoka and T. Makita |
425-436 | The vapor pressure of indium, silver, gallium, copper, tin, and gold between 0.1 and 3.0 bar | F. Geiger, C. A. Busse and R. I. Loehrke |
437-447 | Hydrogen component fugacities in binary mixtures with ethane: Temperature dependence | T. J. Bruno and J. A. Schroeder |
449-471 | Statistical mechanical description of supercritical fluid extraction and retrograde condensation | S. J. Park, T. Y. Kwak and G. A. Mansoori |
473-480 | Determination of the elastic moduli of a machinable ceramic over the range from room temperature to 800°C | H. Nakano, S. Nagai and H. Imai |
481-510 | Critical evaluation of the thermodynamic properties of cobalt | A. Fernández Guillermet |